WO1997012376A1 - Procede de regulation des caracteristiques d'amplitude et de phase d'onde regulation - Google Patents

Procede de regulation des caracteristiques d'amplitude et de phase d'onde regulation Download PDF

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Publication number
WO1997012376A1
WO1997012376A1 PCT/BY1996/000009 BY9600009W WO9712376A1 WO 1997012376 A1 WO1997012376 A1 WO 1997012376A1 BY 9600009 W BY9600009 W BY 9600009W WO 9712376 A1 WO9712376 A1 WO 9712376A1
Authority
WO
WIPO (PCT)
Prior art keywords
aτοmοv
wave
chτο
atomic
vοlny
Prior art date
Application number
PCT/BY1996/000009
Other languages
English (en)
Russian (ru)
Inventor
Alexandr Valerievich Soroko
Original Assignee
Alexandr Valerievich Soroko
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Alexandr Valerievich Soroko filed Critical Alexandr Valerievich Soroko
Publication of WO1997012376A1 publication Critical patent/WO1997012376A1/fr

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Classifications

    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H3/00—Production or acceleration of neutral particle beams, e.g. molecular or atomic beams
    • H05H3/04—Acceleration by electromagnetic wave pressure
    • G—PHYSICS
    • G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
    • G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
    • G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating

Definitions

  • the beam of the atom is emitted through the discovery of a direct and indirect electromagnetic radiation.
  • ⁇ dna ⁇ in ⁇ lichie ⁇ s ⁇ s ⁇ ba [1] ⁇ aches ⁇ ve ⁇ a ⁇ g ⁇ radiation is ⁇ lzuyu ⁇ su ⁇ e ⁇ zitsiyu ⁇ izv ⁇ ln ⁇ y ⁇ edme ⁇ n ⁇ y and ⁇ l ⁇ s ⁇ y ⁇ n ⁇ y ele ⁇ magni ⁇ ny ⁇ v ⁇ ln, ⁇ uch ⁇ a ⁇ m ⁇ v na ⁇ avlyayu ⁇ vd ⁇ l or ⁇ iv ⁇ n ⁇ y ele ⁇ magni ⁇ n ⁇ y v ⁇ lny and ⁇ luchiv a ⁇ mnuyu v ⁇ lnu, imi ⁇ i ⁇ uyuschuyu ⁇ edme ⁇ nuyu ele ⁇ magni ⁇ nuyu v ⁇ lnu, v ⁇
  • ⁇ ⁇ am ⁇ a ⁇ e ⁇ g ⁇ ⁇ iblizheniya ma ⁇ itsa ⁇ l ⁇ n ⁇ s ⁇ i ⁇ sn ⁇ vn ⁇ g ⁇ s ⁇ s ⁇ yaniya a ⁇ ma on ⁇ m ⁇ iz ⁇ shl ⁇ ⁇ dn ⁇ nn ⁇ e vynuzhdenn ⁇ e ⁇ asseyanie ele ⁇ magni ⁇ ny ⁇ v ⁇ ln, ⁇ i usl ⁇ viya ⁇ , ch ⁇ ⁇ tsess eg ⁇ v ⁇ zbuzhdeniya not zavisi ⁇ ⁇ im ⁇ ulsa, ⁇ ine ⁇ iches ⁇ aya ene ⁇ giya s ⁇ anyae ⁇ sya and s ⁇ m ⁇ ensi ⁇ van ⁇ deys ⁇ vie g ⁇ avi ⁇ atsii, ⁇ inima
  • ⁇ is the mass of the atom
  • ⁇ ⁇ is the width of the spectral interval in the short run; ⁇ 97/12376 ⁇ / ⁇ 96 / 00009
  • ⁇ y is the width of the section of the correlation between the child and the general free [4].
  • L is a charac teristic size of the interaction between radiation and the atomic beam in the direction of the dispersion of a small wavelength.
  • the electromagnetic waves are in good condition and satisfy the conditions (5) - (9), (11), (12) may not be emitted.
  • the parameters of the large arrester specify that the pulses of the houses are slightly different from the momentum of the wave or the good result. For this, they use a laser cooling method at temperatures lower than the output energy [5,6]. For the purpose of increasing the length of the free run of particles to values that are much larger than the size of the field and
  • ⁇ ⁇ ) is the total effective cross-section of the dispersion of atoms as the function of energy in the mass center system.
  • e is the charge of the elec- tron
  • t is the mass of the electron
  • EXAMPLE 1 For the local building up of a mixed epithelial layer in the process of creating an integrated tactics of the atomic beam ( ⁇ ) with an instant of 10 ⁇ 97/12376 1 1 ⁇ / ⁇ 96 / 00009
  • the source of electromagnet radiation uses a + g + laser, generating one of the wavelengths ( ⁇ m): 0.4545, 0.4579,
  • Design ⁇ 0 + ⁇ ⁇ is oriented in the positive direction of Axi ⁇ . But on the other hand, there is a polarization of atoms.
  • ⁇ i ⁇ ge is ⁇ blas ⁇ i ⁇ as ⁇ s ⁇ aneniya ⁇ uch ⁇ a ⁇ luchayu ⁇ s ⁇ dyaschuyusya s ⁇ e ⁇ iches ⁇ uyu a ⁇ mnuyu v ⁇ lnu, iden ⁇ ichnuyu ⁇ edme ⁇ n ⁇ y with ⁇ chn ⁇ s ⁇ yu d ⁇ ⁇ s ⁇ yann ⁇ g ⁇ ⁇ m ⁇ le ⁇ sn ⁇ g ⁇ mn ⁇ zhi ⁇ elya and d ⁇ s ⁇ igayu ⁇ , ⁇ a ⁇ im ⁇ b ⁇ az ⁇ m, ⁇ chechn ⁇ g ⁇ ⁇ sazhdeniya a ⁇ m ⁇ v ⁇ imesi on ⁇ lu ⁇ v ⁇ dni ⁇ v ⁇ y ⁇ las
  • the average value of the impulse of the atom is equal to 2.954-U "27 ⁇ s, and
  • the distributed beam receives a convergent spacial wave, an important integrated factor, and it is accepted that

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  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Engineering & Computer Science (AREA)
  • Electromagnetism (AREA)
  • Plasma & Fusion (AREA)
  • General Physics & Mathematics (AREA)
  • General Engineering & Computer Science (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)

Abstract

Cette invention concerne un procédé de régulation des caractéristiques d'amplitude et de phase d'une onde atomique, lequel consiste à envoyer un faisceau d'atomes à travers une zone de rayonnement électromagnétique non uniforme et tridimensionnel obtenu par la superposition de l'onde électromagnétique d'un objet arbitraire et d'une onde électromagnétique de référence plane. Le faisceau d'atomes est orienté le long ou à l'encontre de l'onde électromagnétique de référence et, une fois que l'on a obtenu une onde atomique imitant l'onde électromagnétique de l'objet, on procède à la restitution de l'image de l'objet dans les faisceaux d'atomes. On effectue enfin, dans la zone de dispersion des atomes, un compensation de la pesanteur qui s'exerce sur ces derniers.
PCT/BY1996/000009 1995-09-27 1996-09-18 Procede de regulation des caracteristiques d'amplitude et de phase d'onde regulation WO1997012376A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
BY950863 1995-09-27
BY950863 1995-09-27

Publications (1)

Publication Number Publication Date
WO1997012376A1 true WO1997012376A1 (fr) 1997-04-03

Family

ID=4083678

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/BY1996/000009 WO1997012376A1 (fr) 1995-09-27 1996-09-18 Procede de regulation des caracteristiques d'amplitude et de phase d'onde regulation

Country Status (1)

Country Link
WO (1) WO1997012376A1 (fr)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SU490368A1 (ru) * 1974-02-25 1975-10-30 Казанский Физико-Технический Институт Ан Ссср Способ получени голограмм на полупроводниковом материале
US4279462A (en) * 1978-03-09 1981-07-21 Sentralinstitutt For Industriell Forskning Method of holographic processing of waves
EP0303355A2 (fr) * 1987-08-10 1989-02-15 Polaroid Corporation Hologrammes et réseaux de diffraction

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SU490368A1 (ru) * 1974-02-25 1975-10-30 Казанский Физико-Технический Институт Ан Ссср Способ получени голограмм на полупроводниковом материале
US4279462A (en) * 1978-03-09 1981-07-21 Sentralinstitutt For Industriell Forskning Method of holographic processing of waves
EP0303355A2 (fr) * 1987-08-10 1989-02-15 Polaroid Corporation Hologrammes et réseaux de diffraction

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